Christoph Haederli - Les thèses en ligne de l'INP - Institut National ...
Christoph Haederli - Les thèses en ligne de l'INP - Institut National ...
Christoph Haederli - Les thèses en ligne de l'INP - Institut National ...
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3-L DC Link ML Converter Properties 71<br />
art, which are making use of the NP curr<strong>en</strong>t – voltage characteristics can also be used for any of the<br />
proposed split DC-link topologies. This finding is rather important, as the published concepts are<br />
numerous and they can both be used as basis for the further <strong>de</strong>velopm<strong>en</strong>t of control schemes and<br />
for the basic un<strong>de</strong>rstanding of the ML converter properties.<br />
The standard NP curr<strong>en</strong>t function common for all 3-L DC link converters can be expressed as:<br />
i = ( 1−<br />
abs(<br />
s))<br />
*<br />
(45)<br />
NP<br />
i out<br />
With the average switching function s from -1 to 1. Alternatively, the per phase duty cycle α L<br />
can be used resulting in:<br />
i = ( 1−<br />
abs(2α −1))<br />
* i<br />
(46)<br />
NP<br />
L<br />
out<br />
4.7 NP curr<strong>en</strong>t in multiphase systems<br />
The findings from the previous paragraph on single phase leg properties can be used for the<br />
investigation of multi phase systems. The NP curr<strong>en</strong>ts in function of the voltage in single phase legs<br />
(45) and (46) combine into characteristic NP curr<strong>en</strong>ts in function of the CM voltage for a giv<strong>en</strong><br />
DM output voltage. Based on the basic NP curr<strong>en</strong>t functions, an analysis of the NP curr<strong>en</strong>t<br />
spectrum can be ma<strong>de</strong>. Specifically, the DC NP curr<strong>en</strong>t term relevant for NP voltage control can be<br />
<strong>de</strong>termined in function of line curr<strong>en</strong>ts and converter switching functions.<br />
4.7.1 NP curr<strong>en</strong>t in function of CM<br />
4.7.1.1 H-bridge<br />
In an H-bridge configuration, a single phase output voltage is created by connecting a load<br />
betwe<strong>en</strong> two single phase legs. The output voltage is proportional to the differ<strong>en</strong>ce of the two<br />
average switching functions s<br />
a<br />
and s b<br />
. The two curr<strong>en</strong>ts sum up to zero, as there is one single<br />
curr<strong>en</strong>t loop.<br />
U<br />
U<br />
= sDM<br />
(47)<br />
2<br />
2<br />
DC<br />
DC<br />
u<br />
out<br />
uout<br />
_ a<br />
− uout<br />
_ b<br />
= *( sa<br />
− sb)<br />
= *<br />
i<br />
out _ a<br />
= −i<br />
(48)<br />
out _ b<br />
i<br />
NP<br />
a<br />
= i ((1 − abs(<br />
s )) − (1 − abs(<br />
s ))) = i * ( abs(<br />
s ) − abs(<br />
s )) (49)<br />
out _ a<br />
*<br />
a<br />
b out _ a<br />
s ≤ * s<br />
(50)<br />
a<br />
0 ∧ sb<br />
≤ 0 → iNP<br />
= iout<br />
_ a<br />
*( sa<br />
− sb)<br />
= iout<br />
_ a<br />
s ≥ * s<br />
(51)<br />
a<br />
0 ∧ sb<br />
≥ 0 → iNP<br />
= iout<br />
_ a<br />
* ( sb<br />
− sa<br />
) = −iout<br />
_ a<br />
s ≥ * 2*<br />
s<br />
(52)<br />
a<br />
0 ∧ sb<br />
≤ 0 → iNP<br />
= −iout<br />
_ a<br />
*( sb<br />
+ sa<br />
) = −iout<br />
_ a<br />
s ≤ * 2*<br />
s<br />
(53)<br />
0 ∧ sb<br />
≥ 0 → iNP<br />
= iout<br />
_ a<br />
*( sb<br />
+ sa<br />
) = iout<br />
_ a<br />
DM<br />
DM<br />
CM<br />
b<br />
CM<br />
a